CATADIOPTRIC IMAGING SYSTEMS FOR DIGITAL SCANNER

Abstract

Projection optical system for forming an image on a substrate and including an illumination relay lens and a projection lens each of which is a catadioptric system. The projection lens may include two portions in optical communication with one another, the first of which is dioptric and the second of which is catadioptric. In a specific case, the projection optical system satisfies 4 <  β I   β T  < 30 , where βI and βT are magnifications of the first portion and the overall projection lens. Optionally, the projection lens may be structured to additionally satisfy 6 <  β II   β T  < 20 , where βII is a magnification of the second portion. A digital scanner including such projection optical system and operating with UV light having a spectral bandwidth on the order of 1 picometer. Method for forming an image with such projection optical system.

Description

CROSS-REFERENCE TO RELATED APPLICATIONS

The present application is a continuation-in-part from the U.S. patent application Ser. No. 14/550,465 filed on Nov. 21, 2014 and titled “Catadioptric Imaging Systems for Digital Scanner”, which in turn claims benefit of and priority from the U.S. Provisional Patent Application No. 61/907,747 filed on Nov. 22, 2013 and titled “Catadioptric Imaging Systems for Digital Scanner”. The disclosure of the above-mentioned provisional application is incorporated herein by reference.

TECHNICAL FIELD

The present invention relates generally to lithographic projection optics such as that, which may be used to form an image of a reticle on a semiconductor wafer used in semiconductor manufacturing and, in particular, to lithographic projection optics that are designed to operate with numerical aperture equal to or exceeding 1.0.

BACKGROUND

Chromatic aberrations of optical projection systems that utilize refractive optical elements understandably depend on the bandwidth of light used for projecting an image of a chosen object and, depending on the severity of such aberrations, may require complex designs for aberration compensation. It may be necessary to correct chromatic aberrations for broader bandwidth of light depending on the type of light source.

Attempts were made to address the loss-of-image-contrast problem by devising such projection systems that employ an SLM and that are built around the use of a projection optics containing a catadioptric sub-portion. The proposed optical projection systems can be viewed as including two main portions or sub-systems: a first portion structured as an illumination relay configured to deliver light from a light source to the SLM and to perform what in the art is referred to as “field framing”, and a second portion configured to project the light distribution from the plane of the SLM onto the image plane (the wafer) and referred to as a projection sub-system. While a projection sub-system was proposed to be structured as a catadioptric system, the illumination relay is kept conventionally dioptric (which causes, notably, an overall optical projection system to be sometimes impractically long, unless the optical path is intentionally folded with plane mirrors). It is recognized that the existing solutions still require improvements with respect to several operationally important aspects.

Accordingly, at least the greater-than-acceptable levels of chromatic aberrations in existing projection systems and insufficient reduction ratios define a need in redesign of an optical projection system for efficient use in conjunction with a digital scanner.

SUMMARY

Embodiments of the invention provide a projection optical system configured to form an image on a substrate and including a catadioptric illumination relay lens and a catadioptric projection lens. A projection optical system may include a spatial light modulator (SLM) positioned to receive light from the catadioptric illumination relay lens and reflect said light towards the catadioptric projection lens.

Embodiments additionally provide a projection optical system for forming an image on an image plane, which system contains a catadioptric projection lens that includes first and second portions in optical communication with one another; the second portion is configured as a catadioptric optical system designed to form an intermediate optical image at a location between the elements of the second portion; the first portion is configured as a dioptric optical system disposed to transfer light from the location of the intermediate optical image to the image plane of the projection optical system to form the image at the image plane. The catadioptric projection lens is structured to satisfy an operational condition of

$4<\frac{{\beta }_I}{{\beta }_T}<30,$

wherein β_I denotes a magnification of the first portion and β_T denotes a magnification of the catadioptric projection lens.

Embodiments of the invention additionally provide a projection optical system for forming an image on an image plane. Such system includes a catadioptric projection lens that contains first and second portions in optical communication with one another, where the second portion is designed as a catadioptric optical system configured to form an intermediate optical image at a location between the elements of the second portion. At the same time, the first portion is designed as a dioptric optical system and is disposed such as to transfer light from the location of the intermediate image to the image plane of the projection optical system. The catadioptric projection lens is configured to satisfy an operational condition of

$6<\frac{{\beta }_{\mathrm{II}}}{{\beta }_T}<20,$

wherein β_II denotes a magnification of the second portion and β_T denotes a magnification of the catadioptric projection lens.

Yet another embodiment provides a projection optical system for forming an image on an image plane and including a catadioptric projection lens the first and second portions of which are in optical communication with one another. Here, the second portion is configured as a catadioptric optical system that includes first and second negative lenses and a concave mirror to form an intermediate optical image at a location between the elements of the second portion, while the first portion is configured as a dioptric optical system disposed to form an image of the intermediate optical image at the image plane. The first negative lens has concave and convex surfaces, the concave surface of the first negative lens facing away from the concave mirror. A concave surface of the second negative lens is immediately adjacent to the concave mirror.

BRIEF DESCRIPTION OF THE DRAWINGS

The invention will be more fully understood by referring to the following Detailed Description in conjunction with the generally not-to-scale schematic Drawings, of which:

FIG. 1A is a diagram illustrating a conventionally-structured optical imaging system delivering light from a filed framing plane through an SLM and containing an 0.5× dioptric illuminator relay and a 50× catadioptric projection lens;

FIG. 1B is a diagram illustrating a first portion of the catadioptric projection lens of the embodiment of FIG. 1A;

FIG. 1C is a diagram illustrating a second portion of the catadioptric projection lens of the embodiment of FIG. 1A;

FIG. 1D is a diagram providing details of the dioptric illuminator relay of the embodiment of FIG. 1A;

FIG. 2A is a diagram of an optical imaging system according to an embodiment of the invention structured to deliver light from a filed framing plane through an SLM and containing the same 50× catadioptric projection lens as the embodiment of FIG. 1A but in which the illuminator relay is structured as a 0.5× catadioptric sub-system;

FIG. 2B is a diagram providing details of the catadioptric illuminator relay of the embodiment of FIG. 2A;

FIG. 3A is a diagram illustrating a conventionally-structured optical imaging system delivering light from a filed framing plane through an SLM and containing an 0.5× dioptric illuminator relay and a 200× catadioptric projection lens;

FIG. 3B is a diagram illustrating the catadioptric projection lens of the embodiment of FIG. 3A;

FIG. 3C is a diagram providing details of the dioptric illuminator relay of the embodiment of FIG. 3A;

FIG. 4 is a diagram of an optical imaging system according to an embodiment of the invention structured to deliver light from a filed framing plane through an SLM and containing the same 200× catadioptric projection lens as the embodiment of FIG. 3A but in which the illuminator relay is structured as a 0.5× catadioptric sub-system;

FIG. 5A shows plots representing ray aberrations, within a defined spectral bandwidth around the operating wavelength, at a plane of the SLM (element 24) of the embodiment of FIG. 1A;

FIG. 5B shows plots representing ray aberrations, within a defined spectral bandwidth around the operating wavelength, in the image plane (wafer) of the embodiment of FIG. 1A;

FIG. 6 shows plots representing ray aberrations, within a defined spectral bandwidth around the operating wavelength, in the image plane (wafer) of the embodiment of FIG. 2A;

FIG. 7A shows plots representing ray aberrations, within a defined spectral bandwidth around the operating wavelength, at a plane of the SLM (element 24) of the embodiment of FIG. 3A;

FIG. 7B shows plots representing ray aberrations, within a defined spectral bandwidth around the operating wavelength, in the image plane (wafer) of the embodiment of FIG. 3A;

FIG. 8 shows plots representing ray aberrations, within a defined spectral bandwidth around the operating wavelength, in the image plane (wafer) of the embodiment of FIG. 4;

FIG. 9 is a schematic diagram illustrating a concept of an exposure device (digital scanner) utilizing an embodiment of the invention.

FIG. 10 is a flow-chart illustrating a method for forming an optical image with an embodiment of the projection optical system.

DETAILED DESCRIPTION

Embodiments of the invention provide a projection optical system for forming an image on a substrate and including a catadioptric illumination relay lens and a catadioptric projection lens. A projection optical system may include a spatial light modulator (SLM) positioned to receive light from the catadioptric illumination relay lens and reflect said light towards the catadioptric projection lens. The numerical aperture of the projection optical system is equal to or exceeds 1.0, while the image is formed with a size reduction ratio of at least 50×. When structured to operate at such reduction ratio and in UV light having a central wavelength of about 193.3 nm and a spectral bandwidth of about 1 picometer, the operation of the projection system is characterized by a first Strehl ratio at the central wavelength and a second Strehl ratio across the spectral bandwidth, both of which exceed 0.95. When structured to operate at a reduction ratio of 200× and in the same UV light, both the first and second Strehl ratios exceed 0.98. Embodiments also provide a digital scanner comprising such projection optical system.

Embodiments of the present invention provide a solution for the lack of a hyper-NA (i.e., with NA values exceeding 1.0 and equal to, for example, 1.35) high reduction ratio (50× to 200×, for example) optical projection system configured for efficient use with a digital scanner, which system is operable, for practical lithographic purposes, across a spectral bandwidth of light on the order or 1 pm without substantial loss of image contrast caused by chromatic aberrations. Embodiments include optical projection systems in which both the illumination relay sub-portion and the projection sub-portion are catadioptric.

While one can attempt to argue that the precise and accurate performance of the projection sub-system (i.e., a sub-system of the overall projection system that re-images light from the SLM onto the wafer) may be more critical than that of the illumination relay sub-system because the actual semiconductor circuit structure is produced by reimaging the SLM onto the wafer, the design data discussed below prove that continued utilization of a conventionally dioptrically-designed illumination relay sub-system leads to substantial underperformance of the overall projection system.

Specifically, a comparison of operational characteristics of (i) a conventional projection system including a 0.5× dioptric illumination relay subsystem (interchangeably referred to herein as an “illuminator relay”) and a 50× catadioptric projection sub-system (interchangeably referred to herein as a “catadioptric projection lens”) and those of (ii) an embodiment of the present invention including a 0.5× catadioptric illuminator relay and a 50× catadioptric projection lens is provided. Also are analyzed (and compared with one another) operational characteristics of (iii) a conventionally-designed system combining a 0.5× dioptric illuminator relay with a 200× catadioptric projection lens and those of (iv) an embodiment of the invention combining the 0.5× dioptric illuminator relay with a 200× catadioptric projection lens.

Several additional notes are in order for ease of understanding of the following disclosure. Tables 1 through 4 in the following discussion summarize the prescriptions for designs of various optical systems and their subsystems that were performed with Code V and that are discussed in reference to corresponding Figures. In these Tables, optical elements are numbered in a “backward” fashion, starting with the semiconductor wafer (defining the image plane) towards the source of light, which makes it easier, as would be appreciated by a skilled artisan, to define the NA and telecentricity in wafer space during the process of optical design. The semiconductor wafer (with a wafer plane labeled as 1 in the Tables) is submerged in fluid (for example, water, as shown in inset of FIG. 1B) that separates the closest lens (marked as element 2 in the Tables) from it. This condition applies to each of the presented embodiments. Positive radius value indicates that the center of curvature is to the right, while a negative radius value indicates that the center of curvature is to the left; dimensions are provided in millimeters; thickness is defined as an axial distance to the next surface; and an indicated image diameter is a paraxial value and not a ray traced value. Furthermore, with respect to decentering constants, a decenter defines a new coordinate system (displaced and/or rotated) in which subsequent surfaces are defined. Surfaces following a decenter are aligned on the local mechanical axis (z-axis) of the new coordinate system. The new mechanical axis remains in use for referencing purposes until expressly changed by another decenter. The order in which displacements and tilts are applied to a given surface is specified using different decenter types and these generate different new coordinate systems; those used in this disclosure are explained below. Alpha, beta, and gamma values are presented in degrees. Additionally, with respect to chromatic aberrations, a reduction in Strehl ratio between monochromatic and polychromatic deigns represents the contrast loss from chromatic aberrations over the specified spectral band, while a variation in best individual focus shows the residual field curvature.

An embodiment of the catadioptric optical projection system according to the invention is designed to ensure, in operation, at least a 50× reduction ratio and is characterized by a hyper-NA (of at least 1.0) catadioptric projection lens and an instantaneous line field of view (one dimensional, 1D, FOV) of about 3.6 mm on the surface of the wafer. The projection optical system is structured to be compatible with principles of maskless lithography, according to which the conventionally used mask (or reticle) is replaced by an SLM. The SLM may take a form of a 1D array of microelectromechanical actuators, or MEMS, for example, or actuators on the scale of a few tens or hundreds of nanometers (NEMS). U.S. Pat. Nos. 5,312,513; 5,523,193; 7,110,082; 7,206,117; 7,952,780; and 2013/0003166, the disclosure of each of which is incorporated by reference herein, provide additional information on SLM technology.

Example 1

Catadioptric Embodiment with a 50× Reduction Ratio

FIGS. 1A, 1B, 1C, and 1D illustrate an optical imaging system 100 providing a 50× reduction ratio and structured conventionally in that, while the projection lens portion (I and II) includes a catadioptric optical system, the illumination relay portion (III) is dioptric. To illustrate contradistinctively advantageous operational characteristics of a fully-catadioptric system configured according to an embodiment of the present invention, a comparison is made with a 50×-reducing optical system of FIGS. 2A and 2B, in which each of the projection lens portion (I and II) and the illuminator relay (III-CAT) is structured as a catadioptric system. For the purposes of comparison, the projection lens portions of both the system of FIG. 1A and the embodiment of FIG. 2A are identical.

As shown in FIG. 1A, the illumination relay III images a field framing plane (element 33 that is illuminated with a telecentric system, not shown) onto the plane of the SLM (element 24) with a 2× magnification. The light-beam 110 further passes, upon reflection from the SLM (element 24), without obscuration into the catadioptric projection sub-system (II and I) that reduced the image on the surface of the wafer (element 1) by 50×. FIGS. 1B, 1C, and 1D show the details of sub-portions of the embodiment 100.

As shown in FIG. 2A, the embodiment 200 of the present invention includes the catadioptric projection sub-system (the combination of II and I) that is the same as in the embodiment 100, operably concatenated with the catadioptric illumination relay (III-CAT). The catadioptric illumination relay III-CAT images a field framing plane (element 34 that is illuminated with a telecentric system, not shown) onto the plane of the SLM (element 24) with a 2× magnification. The light-beam 210 further passes, upon reflection from the SLM (element 24), without obscuration into the catadioptric projection sub-system (II and I) that reduced the image on the surface of the wafer (element 1) by 50×. The resulting size of the rectangular image on the wafer surface is about 3.6×0.16 mm², which corresponds to about 180×8 mm² light distribution at the plane of the SLM and to about 90×4 mm² at the field framing plane (element 34). Optionally, blades may be utilized in the field framing plane to define sharply and/or further limit the size of the field. FIG. 2B shows the details of the optical train of the catadioptric illuminator relay III-CAT.

In both embodiments 100 and 200 (FIGS. 1A and 2A, respectively), the long dimension of the field is extended perpendicularly to the plane of the drawing (or parallel to the x-axis, as indicated). In both embodiments 100 and 200, the SLM (element 24) contains a 1D array of microreflectors that is perpendicular to the plane of the corresponding drawings and is slightly more than 180 mm in length. In both embodiments the SLM is illuminated through the corresponding illumination relay (III, III-CAT) with light delivered from a high-repetition (˜1 MHz) UV laser source having a specified spectral bandwidth around the central wavelength of about 193 nm. The laser source used for SLM-utilizing projection optical system of the invention has a bandwidth that is about 30-fold that of a typical UV excimer laser (employed with a conventional scanner used in lithography), and has a repetition rate exceeding that of the excimer laser by about three orders of magnitude. The detailed Code V description of the optical train of the embodiment 100 is presented in Table 1A, while the corresponding description of the optical train of the embodiment of the invention 200 is presented in Table 2A.

In comparison with the design of the illumination relay III of the embodiment of FIG. 1A, and as detailed in Table 2A, the catadioptric illumination relay III-CAT includes a spherical mirror (element 29). The catadioptric projection lens (I, II) of either embodiment 100 or 200 also comprises a spherical mirror and a fold mirror (elements 14, 18), but in addition forms an intermediate image close to the fold mirror (element 14) and a number of aspheric lens elements (such as, for example, elements 13, 15, 17) that, in conjunction with the relay III-CAT, facilitate hyper-NA of 1.35 at the immersed in water wafer surface.

Descriptions of aberrations characterizing imaging through the catadioptric lens I, II of the embodiment 100 of the field framing plane 33 of the embodiment 100 of FIG. 1A onto the surface of the wafer 1 are presented in FIG. 5A and Tables 1B, 1C. Table 1B addresses the ray aberrations at the plane of the SLM (at wavelengths in an approximately 3 pm-wide spectral bandwidth centered at about 193.3 nm), and wavefront aberrations associated with the imaging through the catadioptric lens I, II of the embodiment 100). Table 1C addresses the wavefront aberrations associated with the imaging through the overall optical system of the embodiment 100, between the field framing plane 33 of the embodiment 100 and the surface of the wafer 1. FIG. 5B complements the data of FIG. 1A by providing lots of ray aberrations defined, for the embodiment of FIG. 1A, in the image plane (wafer) within a defined spectral bandwidth around the operating wavelengths. Descriptions of aberrations characterizing imaging through the overall optical system of the embodiment 200 of the invention, between the field framing plane 34 of the embodiment 200 and the surface of the wafer 1 of FIG. 2A, are summarized in FIG. 6 and Table 2B (addressing the ray aberrations and wavefront aberrations, respectively). The direct comparison between the data on aberrations for the fully-catadioptric projection lens according to the idea of the invention with those for a conventional lens highlights the advantages of the embodiment of the invention, as would be recognized by a skilled artisan.

A person of skill in the art will readily appreciate, from the data of Tables 2B and 1C, for example, that the field curvature of the fully-catadioptric design of the invention (shown in a column representing the focus position as a function of field height) is substantially smaller than that of a conventionally-design system 100. Moreover, the difference between the figures of merits describing the polychromatic aberrations and those describing monochromatic aberrations is substantially smaller for the embodiment 200 of the invention as compared to the embodiment 100. Furthermore, the values of Strehl ratio across the field for the embodiment 200 of the invention are substantially higher than those for the embodiment 100 (see, for example, Strehl ratios respectively characterizing monochromatic rms wavefront aberrations). The embodiment of the invention ensures, in addition to operationally negligible distortion of imaging between the SLM and the wafer, very small residual monochromatic aberrations on the order of about 5 milliwaves rms or less.

Example 2

Catadioptric Embodiment With 200× Reduction Ratio

FIGS. 3A, 3B, 3C illustrate an optical imaging system 300 providing a 200× reduction ratio and structured conventionally in that, while the projection lens portion (A) includes a catadioptric optical system, the illumination relay portion (B) is conventionally dioptric. To illustrate contradistinctively advantageous operational characteristics of a fully-catadioptric system according to an embodiment of the present invention, a comparison is made with a 200×-reducing optical system of FIG. 4, in which both the projection lens portion (A) and the illuminator relay (B-CAT) are structured as catadioptric systems. For the purposes of the comparison, the projection lens portions of both the system of FIG. 3A and the embodiment of FIG. 4 are identical. FIGS. 3B and 3C show the details of sub-portions of the embodiment 300.

As shown in FIG. 4, the embodiment 400 of the present invention includes the catadioptric 200×-reduction projection sub-system (A) that is the same as that of the embodiment 300, concatenated with the catadioptric illumination relay B-CAT that images a field framing plane (element 33, illuminated with a telecentric system, not shown) onto the plane of the SLM (element 24) with a 2× magnification. The resulting size of the rectangular image on the wafer surface (1) is about 0.64×0.16 mm², which corresponds to about 128×32 mm² light distribution at the plane of the SLM and to about 64×16 mm² at the field framing plane (element 33). Optionally, blades may be utilized in the field framing plane to define sharply and/or further limit the size of the field. FIG. 2B shows the details of the optical train of the catadioptric illuminator relay III-CAT. In both embodiments 300 and 300 (FIGS. 1A and 2A, respectively), the long dimension of the field is perpendicular to the plane of the drawing (or parallel to the x-axis, as indicated). The parameters of illuminating UV light used to design the optical trains of the embodiment 300 (presented in Table 3A) and the optical train of the embodiment of the invention 400 (presented in Table 4A) are the same as those discussed in reference to FIGS. 1A, 2A.

In comparison with the design of the illumination relay B of the embodiment 300 of FIG. 3A, and as detailed in Table 4A, the catadioptric illumination relay B-CAT includes one spherical mirror (element 29) and one extra fold planar mirror (element 28). The catadioptric projection lens (A) of either embodiment 300 or 400 also comprises a spherical mirror and a fold mirror, but in addition forms an intermediate image close to the fold mirror (element 14) and a number of aspheric lens elements that, in conjunction with the relay B-CAT, facilitate hyper-NA of 1.35 for the fully-catadioptric embodiment 400 at the immersed in water wafer surface.

Descriptions of aberrations characterizing imaging through the catadioptric lens A of the embodiment 300 of the field framing plane 32 onto the surface of the wafer 1 are presented in FIG. 7A and Table 3B (addressing the ray aberrations, at wavelengths in an approximately 3 pm-wide spectral bandwidth centered at about 193.3 nm, at the plane of the SLM and wavefront aberrations associated with the imaging through the catadioptric lens A of the embodiment 300) and Table 3C (addressing the wavefront aberrations associated with the imaging through the overall optical system of the embodiment 300, between the field framing plane 32 and the surface of the wafer 1). FIG. 7B complements the data of FIG. 7A by providing lots of ray aberrations defined, for the embodiment of FIG. 3A, in the image plane (wafer) within a defined spectral bandwidth around the operating wavelengths. Descriptions of aberrations characterizing imaging through the overall optical system of the embodiment 400 of the invention, between the field framing plane 33 of the embodiment 400 and the surface of the wafer 1 of FIG. 4, are summarized in FIG. 8 and Table 4B (addressing the ray aberrations and wavefront aberrations, respectively). The direct comparison between the data on aberrations for the fully-catadioptric projection lens according to the idea of the invention with those for a conventional lens highlights the advantages of the embodiment of the invention.

As evidenced by the disclosed data, a person of skill in the art will readily appreciate that, for example, the field curvature of the fully-catadioptric design of the invention is substantially reduced compared to that of a conventionally-design system 300. Moreover, the difference between the figures of merits describing the polychromatic aberrations and those describing monochromatic aberrations is substantially smaller for the embodiment 400 of the invention as compared to the embodiment 300. Furthermore, the values of Strehl ratio across the field for the embodiment 400 of the invention are substantially higher than those for the embodiment 300 (see, for example, Strehl ratios respectively characterizing monochromatic rms wavefront aberrations). The embodiment of the invention ensures, in addition to operationally negligible distortion of imaging between the SLM and the wafer, very small residual monochromatic aberrations on the order of about 5 milliwaves rms or less.

It is worth noting that, by structuring the illumination relay of the overall projection system as a catadioptric sub-system, the chromatic aberrations of imaging are substantially reduced in the 50× to 200× dimension reduction system that employs only fused silica refractive optical elements and without the use of complex lenses employing 3 different materials (such s, for example, a classical doublet lens). The reduction of chromatic aberrations results in negligible loss of image contrast when an embodiment of the invention—as compared to a conventionally-designed dioptric-catadioptric projection system—when the system is used with a solid-state laser source the spectral bandwidth of which is on the order of 1 pm FWHM.

Accordingly, embodiments of the present invention provides maskless projection optical systems structured to enable imaging of an object pattern onto a semiconductor wafer with a de-magnification factor of at least 50× and as high as 200×. The projection optics comprises an illumination relay, which projects the UV light of about 193 nm from a field framing plane onto the SLM that reflects the incident light, and a projection lens through which the SLM-reflected UV light is further directed to a semiconductor substrate. The SLM is illuminated by non-telecentric off-axis illumination, and both the illumination relay and the projection lens include a catadioptric optical sub-system to advantageously reduce chromatic aberrations of the system operating in a spectral bandwidth on the order of 1 pm. A fluid is provided between the substrate and the last optical element of the projection lens. The projection optical systems of the invention are configured to enable imaging with an NA of 1.0 or higher.

Example of a Wafer Exposure Apparatus.

An embodiment 900 of the exposure apparatus utilizing an embodiment of the invention is shown in a diagram of FIG. 9, and is equipped with an illumination system 910, a pattern generation device 112, the fully-catadioptric imaging system 902 (such as, for example, an embodiment 200 or 400), a positioning stage device 916, an electronic circuitry governing these and other devices. FIG. 9 illustrates only a schematic of the embodiment, approximately indicating the operable cooperation among the components of the apparatus and not the precise position or orientation of such components, and is not to scale. The exposure apparatus 900 performs an exposure process by projecting an image of a pattern, which is generated by the pattern generation device 112, on a wafer plate (sensitive substrate) W mounted on a stage ST that constitutes a part of the stage device 916, via the catadioptric system of the invention 902, in a scanning fashion that includes synchronization of switching (changing) of a pattern generated by the pattern generation device 912 with movement of the wafer W. The wafer W is scanned in the xy-plane as indicated, with the SLM plane being perpendicular to the plane of the wafer. The exposure apparatus has a degree of freedom to change the angular orientation of the wafer W about the x, y, and z-axes.

The control system includes a data-collection and/or data-processing electronic circuitry (controller) 920 that may be part of a computer processor specifically programmed to govern the operation of the apparatus 900. The control system may be connected to a host device 950 via a communication interface 932.

The illumination system 910 delivers preferably spatially-uniform illumination of a variable molding mask VM, which constitutes a part of the pattern generation device 912, with an illumination (exposure)) UV-light IL, and is equipped with: a light source system including at least a UV-light source and a light source control system and an illumination condition-setting mechanism operable to change changing light irradiance distribution at the pupil plane of the illumination optical system; optionally a field stop, a relay lens, and other required zooming, polarizing optical elements as required, among which there may be present an optical integrator (a fly-eye lens), not shown.

The pattern generation device 912 is an electronic mask system that generates a variable pattern to be projected onto the waver W mounted on the stage ST, and is equipped with at least: the variable molding mask VM; a holder 928 that holds the variable molding mask VM; a drive system (controller) 930 that controls operation states of the variable molding mask VM; a tangible, non-transitory and optionally computer-readable memory 933. The mask variable molding mask may generally include a device containing a plurality of micro-reflectors such as, for example, a digital micro-mirror device, known as a DMD, or a 3D MEMS.

The variable molding mask VM is placed above (+Z side) the fully-catadioptric embodiment of the projection system 902, and the illumination light IL is delivered to the system 902 from the illumination system 110 upon reflection from the variable molding mask.

The drive system 930 acquires design data (such as CAD data) of a pattern, required for forming a pattern image on the wafer W, from the host device 950 via the interface 932. The drive system 930 further refers to data (hereinafter, called “signal generation information”) stored in the memory 933, and generates signals to drive the elements/mirrors of the variable molding mask VM based on the design data acquired. The signals to drive each micro mirror are supplied to the driving mechanism of each micro mirror. The drive system 930 can vary patterns to be generated by the variable molding mask VM based on the design data acquired, which may be optionally effectuated synchronously with the movements of the wafer W P mounted on the stage ST.

In addition to the elements of the fully-catadioptric projections system 902 discussed above in reference to the embodiments of FIGS. 2A and 4, an image-forming property compensation device 938 (which drives particular elements inside the fully-catadioptric system 902 in the directions Ax1 AX2 and tilts them according to the provided degrees of angular freedom) may be arranged in operable communication with the system 902. The image-forming property compensation device 938 adjusts image-forming states of the fully catadioptric system 902 of the invention. Alternatively or in addition, wavelength properties of the illumination light IL (such as center of wavelength, spectral bandwidth, and the like) may be controlled to achieve the modification of the image on the wafer W.

The stage device 916 is equipped with: the stage ST that is movable while holding a wafer W (such as a glass substrate, a semiconductor wafer, for example) prepared for exposure; and a stage drive system 940 that controls the operational states (movement and the like) of the stage ST according to commands received from the main controller 920. Positional information (including rotation information) describing the orientation of the stage ST is measured by a positional measurement system (not shown) that may include, for example, a laser interferometer and/or encoder as well as a focus sensor, and is supplied to the main controller 920 which, in turn, drives motors of the stage drive system 940 based on such positional information.

TABLE 1A
Description of Optical Train of the Embodiment 100 of FIG. 1A.
ELEMENT	RADIUS OF CURVATURE		APERTURE DIAMETER
NUMBER	FRONT	BACK	THICKNESS	FRONT	BACK	GLASS
OBJECT	INF	3.0000			‘Water’
2	INF	−16.2570	CX	13.1558	20.2277	30.2121	‘SiO2’
				0.2869
3	S(1)	−39.7263	CX	15.3707	46.7684	59.3550	‘SiO2’
				0.2869
4	S(2)	−60.2724	CX	19.0464	76.1508	82.8331	‘SiO2’
				APERTURE STOP	82.8331
				0.2869
5	S(3)	−76.5071	CX	18.2258	90.6356	96.6083	‘SiO2’
			0.5739
6	359.3759	CX	S(4)	23.0773	104.8449	106.5348	‘SiO2’
				37.1856
7	308.2081	CX	−328.8230	CX	26.5407	102.9433	99.8443	‘SiO2’
					12.2840
8	89.4404	CX	1362.2325	CC	16.7807	87.4584	83.3926	‘SiO2’
				8.8213
9	S(5)	−487.6829	CX	7.5000	81.5244	78.3413	‘SiO2’
				76.8018
10	193.1846	CX	71.5006	CC	5.0000	38.8226	36.4073	‘SiO2’
				7.6993
11	−39.8835	CC	A(1)	5.0000	36.1057	38.1009	‘SiO2’
				33.5985
12	382.1002	CX	−77.5554	CX	12.0926	53.9990	55.5152	‘SiO2’
				1.0000
13	1310.5028	CX	A(2)	8.5747	55.3320	55.1363	‘SiO2’
			50.0953
	DECENTER(1)
14	INF	−50.2113	C-1	REFL
15	−524.0530	CX	A(3)	−13.2517	60.2578	61.4956	‘SiO2’
				−206.1572
16	58.8481	CC	115.4857	CX	−5.0000	69.6685	75.0749	‘SiO2’
				−1.1717
17	A(4)	−113.4481	CC	−5.1648	76.6516	81.7457	‘SiO2’
			−123.3907
18	181.5965 CC	123.3907	185.8623	REFL
19	−113.4481	CC	A(5)	5.1648	92.6117	88.5530	‘SiO2’
				1.1717
20	115.4857	CX	58.8481	CC	5.0000	86.0541	79.2534	‘SiO2’
				206.1572
21	A(6)	−524.0530	CX	13.2517	93.7414	93.1676	‘SiO2’
			50.2113
	DECENTER(2)
				88.5989
			49.9344
22	−128.3482	CC	120.3731	CC	14.6614	68.5771	69.6874	‘SiO2’
				107.6287
23	A(7)	−86.2586	CX	11.8617	108.0913	112.2249	‘SiO2’
			502.2967
24	INF	−100.0000	216.3994	REFL
	DECENTER(3)
25	INF	100.0000	C-2	REFL
26	419.9816	CX	−714.1824	CX	44.9407	282.2641	281.7818	‘SiO2’
					0.1000
27	216.9230	CX	167.2850	CC	32.4700	261.3636	234.5263	‘SiO2’
			557.4266
				157.5295
			0.0000
				157.5295
			295.3348
28	127.1564	CX	−23012.2683	CX	51.4661	112.2159	95.5665	‘SiO2’
					95.5116
29	−72.8237	CC	84.6697	CC	11.0413	32.0499	30.0404	‘SiO2’
					27.3428
30	595.1633	CX	−94.4057	CX	76.1582	42.0182	68.6892	‘SiO2’
					341.1608
31	202.9635	CX	−702.1241	CX	35.0000	136.2980	133.6332	‘SiO2’
					0.6118
32	99.8742	CX	80.2315	CC	8.0304	125.3481	117.0218	‘SiO2’
	IMAGE DISTANCE =	123.4048
33 IMAGE	INF		108.1814
APERTURE DATA
		DIAMETER	DECENTER
APERTURE	SHAPE	X	Y	X	Y	ROTATION
C-1	RECTANGLE	52.482	20.000	0.000	25.000	0.0
C-2	RECTANGLE	307.113	40.000	0.000	−110.000	0.0
aspheric constants
$\begin{array}{cc}Z=\frac{\left(\mathrm{CURV}\right)Y^2}{1+{\left(1-\left(1+K\right){\left(\mathrm{CURV}\right)}^2Y^2\right)}^{1/2}}& +\left(A\right)Y^4+\left(B\right)Y^6+\left(C\right)Y^8+\left(D\right)Y^{10}+\left(E\right)Y^{12}+\left(F\right)Y^{14}+\left(G\right)Y^{16}+\left(H\right)Y^{18}+\left(J\right)Y^{20}\end{array}$
		K	A	B	C	D
ASPHERIC	CURV	E	F	G	H	J
A(1)	0.851039E−02	0.00000000	−1.01624E−06	6.08007E−10	−5.62736E−13	1.14084E−15
		−2.32923E−18	2.08999E−21	0.00000E+00	0.00000E+00	0.00000E+00
A(2)	−0.618726E−02	0.00000000	1.39355E−07	1.13165E−11	7.81414E−16	5.66581E−19
		0.00000E+00	0.00000E+00	0.00000E+00	0.00000E+00	0.00000E+00
A(3)	0.518760E−02	0.00000000	−8.99477E−08	−2.67713E−12	−8.56400E−16	7.98734E−20
		0.00000E+00	0.00000E+00	0.00000E+00	0.00000E+00	0.00000E+00
A(4)	0.01015569	0.00000000	−1.65154E−06	−2.76782E−10	1.94297E−13	−5.45936E−17
		8.17140E−21	−4.67186E−25	0.00000E+00	0.00000E+00	0.00000E+00
A(5)	0.01015569	0.00000000	−1.65154E−06	−2.76782E−10	1.94297E−13	−5.45936E−17
		8.17140E−21	−4.67186E−25	0.00000E+00	0.00000E+00	0.00000E+00
A(6)	0.518760E−02	0.00000000	−8.99477E−08	−2.67713E−12	−8.56400E−16	7.98734E−20
		0.00000E+00	0.00000E+00	0.00000E+00	0.00000E+00	0.00000E+00
A(7)	−0.960266E−02	0.00000000	2.22077E−08	1.44665E−12	1.43851E−16	1.09803E−20
		0.00000E+00	0.00000E+00	0.00000E+00	0.00000E+00	0.00000E+00
SPECIAL SURFACES (SPS types)
QCN SURFACES
x = (Y/NRADIUS)**2
$\begin{array}{cc}Z=\frac{\left(\mathrm{CURV}\right)Y^2}{1+{\left(1-\left(1+K\right){\left(\mathrm{CURV}\right)}^2Y^2\right)}^{1/2}}& +x^2*\left(\left(\mathrm{QC}4\right)Q_0^{\mathrm{con}}\left(x\right)+\left(\mathrm{QC}6\right)Q_1^{\mathrm{con}}\left(x\right)+\dots +\left(\mathrm{QC}30\right)Q_{13}^{\mathrm{con}}\left(x\right)\right)\end{array}$
		NRADIUS (C2)
		QC10 (C7)	K (C1)	QC4 (C4)	QC6 (C5)	QC8 (C6)
		QC20 (C12)	QC12 (C8)	QC14 (C9)	QC16 (C10)	QC18 (C11)
ASPHERIC	CURV	QC30 (C17)	QC22 (C13)	QC24 (C14)	QC26 (C15)	QC28 (C16)
S(1)	−0.193296E−01	0.241104E+02	0.000000E+00	0.102350E+01	−0.110831E+00	−0.153148E−01
		0.409086E−02	−0.809714E−03	0.125654E−03	−0.792809E−04	0.106091E−04
		−0.131607E−04	−0.914150E−06	−0.301755E−05	−0.558949E−06	−0.106807E−05
		−0.437373E−06
S(2)	−0.549169E−02	0.410514E+02	0.000000E+00	0.647857E+00	−0.579468E−01	−0.149522E+00
		−0.563430E−01	−0.119113E−01	−0.815318E−02	−0.237721E−02	−0.153527E−02
		−0.416675E−03	−0.202108E−03	−0.522481E−04	−0.187957E−04	−0.238197E−06
		0.192168E−06
S(3)	−0.611446E−02	0.480523E+02	0.000000E+00	0.212139E−01	−0.640452E+00	0.290637E+00
		0.884384E−01	0.160688E−01	−0.316193E−02	−0.469821E−02	−0.111522E−02
		0.393635E−03	0.615198E−03	0.360576E−03	0.142886E−03	0.388167E−04
		0.577816E−05
S(4)	−0.379826E−02	0.559469E+02	0.000000E+00	−0.123020E+01	−0.577347E−01	0.143110E+00
		0.581555E−01	0.175100E−01	0.874534E−02	0.409713E−02	0.198654E−02
		0.915187E−03	0.409889E−03	0.169900E−03	0.634141E−04	0.198459E−04
		0.406977E−05
S(5)	−0.546127E−02	0.430941E+02	0.000000E+00	−0.234582E+01	−0.409559E−01	0.130732E−02
		0.358234E−02	0.144329E−02	0.459955E−03	0.919185E−04	−0.551606E−05
		−0.193417E−04	−0.133179E−04	−0.696762E−05	−0.262871E−05	−0.709265E−06
		0.335430E-07
DECENTERING CONSTANTS
DECENTER	X	Y	Z	ALPHA	BETA	GAMMA
D(1)	0.0000	0.0000	0.0000	45.0000	0.0000	0.0000 (BEND)
D(2)	0.0000	0.0000	0.0000	45.0000	0.0000	0.0000 (RETU)
D(3)	0.0000	0.0000	0.0000	−45.0000	0.0000	0.0000 (BEND)

TABLE 1B
Monochromatic and Polychromatic Wavefront Aberrations and Corresponding Strehl Ratios of the
Catadioptric Projection Lens (I, II) of the Embodiment 100 of FIG. 1A.
	BEST INDIVIDUAL FOCUS	BEST COMPOSITE FOCUS
			SHIFT	FOCUS	RMS		SHIFT	FOCUS	RMS
FIELD	FRACT	DEG	(MM.)	(MM.)	(WAVES)	STREHL	(MM.)	(MM.)	(WAVES)	STREHL
Monochromatic rms wavefront aberrations and Strehl ratio - Wafer to SLM:
X	0.00	0.00	0.000000	0.002182	0.0049	0.999	0.000000	0.000635	0.0050	0.999
Y	1.00	0.00	−0.000058				0.000048
X	0.50	0.00	0.000124	0.002561	0.0050	0.999	0.000025	0.000635	0.0051	0.999
Y	1.00	0.00	−0.000165				−0.000033
X	0.70	0.00	−0.000296	−0.003506	0.0027	1.000	0.000003	0.000635	0.0036	1.000
Y	1.00	0.00	0.000282				−0.000003
X	1.00	0.00	0.000065	0.001322	0.0032	1.000	−0.000005	0.000635	0.0032	1.000
Y	1.00	0.00	−0.000044				0.000003
	COMPOSITE RMS FOR	0.00432
	POSITION 1:
Polychromatic rms wavefront aberrations and Strehl ratio - Wafer to SLM:
Reduction in Strehl ratio between monochromatic and polychromatic cases represents the
contrast loss from chromatic aberrations over the spectral band
WL = 193.3074 193.3069 193.3065 193.306 193.3057 193.3055 193.3046
WTW = 11 29 60 100 69 17 5
X	0.00	0.00	0.000000	0.011497	0.0206	0.983	0.000000	0.009940	0.0206	0.983
Y	1.00	0.00	−0.000054				0.000053
X	0.50	0.00	0.000121	0.011864	0.0207	0.983	0.000022	0.009940	0.0207	0.983
Y	1.00	0.00	−0.000161				−0.000029
X	0.70	0.00	−0.000300	0.005790	0.0204	0.984	−0.000001	0.009940	0.0205	0.984
Y	1.00	0.00	0.000286				0.000001
X	1.00	0.00	0.000063	0.010627	0.0206	0.983	−0.000007	0.009940	0.0206	0.983
Y	1.00	0.00	−0.000042				0.000005
	COMPOSITE RMS FOR POSITION 1:	0.02060

TABLE 1C
Monochromatic and Polychromatic Wavefront Aberrations and Corresponding Strehl Ratios of the Overall
Embodiment 100 of FIG. 1A.
	BEST INDIVIDUAL FOCUS	BEST COMPOSITE FOCUS
			SHIFT	FOCUS	RMS		SHIFT	FOCUS	RMS
FIELD	FRACT	DEG	(MM.)	(MM.)	(WAVES)	STREHL	(MM.)	(MM.)	(WAVES)	STREHL
Monochromatic rms wavefront aberrations and Strehl ratio - Wafer to field framing plane:
Variation in best individual focus shows the residual field curvature.
WL = 193.3074 193.3069 193.3065 193.306 193.3057 193.3055 193.3046
WTW = 0 0 0 1 0 0 0
X	0.00	0.00	0.000000	0.022771	0.0803	0.775	0.000000	−0.007150	0.1047	0.648
Y	1.00	0.00	0.000621				0.000531
X	0.50	0.00	−0.000104	−0.015071	0.0646	0.848	−0.000101	−0.007150	0.0670	0.838
Y	1.00	0.00	0.000133				0.000155
X	0.70	0.00	0.000071	−0.043989	0.0323	0.960	0.000088	−0.007150	0.0877	0.738
Y	1.00	0.00	−0.000050				0.000044
X	1.00	0.00	0.000823	0.007510	0.0866	0.744	0.000816	−0.007150	0.0923	0.714
Y	1.00	0.00	−0.000533				−0.000579
	COMPOSITE RMS FOR POSITION 1:	0.08903
Polychromatic rms wavefront aberrations and Strehl ratio - Wafer to field framing plane:
Reduction in Strehl ratio between monochromatic and polychromatic cases represents the
contrast loss from chromatic aberrations over the spectral band.
Variation in best individual focus shows the residual field curvature.
WL = 193.3074 193.3069 193.3065 193.306 193.3057 193.3055 193.3046
WTW = 11 29 60 100 69 17 5
X	0.00	0.00	0.000000	0.025445	0.0844	0.755	0.000000	−0.004468	0.1079	0.632
Y	1.00	0.00	0.000606				0.000516
X	0.50	0.00	−0.000096	−0.012416	0.0700	0.824	−0.000094	−0.004468	0.0722	0.814
Y	1.00	0.00	0.000118				0.000140
X	0.70	0.00	0.000081	−0.041317	0.0418	0.933	0.000098	−0.004468	0.0916	0.718
Y	1.00	0.00	−0.000064				0.000030
X	1.00	0.00	0.000833	0.010241	0.0902	0.725	0.000827	−0.004468	0.0958	0.696
Y	1.00	0.00	−0.000544				−0.000590
	COMPOSITE RMS FOR POSITION 1:	0.09281

TABLE 2A
Description of Optical Train of the Embodiment 200 of FIG. 2A.
ELEMENT	RADIUS OF CURVATURE		APERTURE DIAMETER
NUMBER	FRONT	BACK	THICKNESS	FRONT	BACK	GLASS
OBJECT	INF	3.0000			‘Water’
2	INF	−16.2570	CX	13.1558	20.2277	30.2121	‘SiO2’
				0.2869
3	S(1)	−39.7263	CX	15.3707	46.7684	59.3550	‘SiO2’
				0.2869
4	S(2)	−60.2724	CX	19.0464	76.1508	82.8331	‘SiO2’
				APERTURE STOP	82.8331
				0.2869
5	S(3)	−76.5071	CX	18.2258	90.6356	96.6083	‘SiO2’
			0.5739
6	359.3759	CX	S(4)	23.0773	104.8449	106.5348	‘SiO2’
				37.1856
7	308.2081	CX	−328.8230	CX	26.5407	102.9433	99.8443	‘SiO2’
					12.2840
8	89.4404	CX	1362.2325	CC	16.7807	87.4584	83.3926	‘SiO2’
				8.8213
9	S(5)	−487.6829	CX	7.5000	81.5244	78.3413	‘SiO2’
				76.8018
10	193.1846	CX	71.5006	CC	5.0000	38.8226	36.4073	‘SiO2’
				7.6993
11	−39.8835	CC	A(1)	5.0000	36.1057	38.1009	‘SiO2’
				33.5985
12	382.1002	CX	−77.5554	CX	12.0926	53.9990	55.5152	‘SiO2’
				1.0000
13	1310.5028	CX	A(2)	8.5747	55.3320	55.1363	‘SiO2’
			50.0953
	DECENTER(1)
14	INF	−50.2113	C-1	REFL
15	−524.0530	CX	A(3)	−13.2517	60.2578	61.4956	‘SiO2’
				−206.1572
16	58.8481	CC	115.4857	CX	−5.0000	69.6685	75.0749	‘SiO2’
				−1.1717
17	A(4)	−113.4481	CC	−5.1648	76.6516	81.7457	‘SiO2’
			−123.3907
18	181.5965 CC	123.3907	185.8623	REFL
19	−113.4481	CC	A(5)	5.1648	92.6117	88.5530	‘SiO2’
				1.1717
20	115.4857	CX	58.8481	CC	5.0000	86.0541	79.2534	‘SiO2’
				206.1572
21	A(6)	−524.0530	CX	13.2517	93.7414	93.1676	‘SiO2’
				50.2113
	DECENTER(2)
				88.5989
			49.9344
22	−128.3482	CC	120.3731	CC	14.6614	68.5771	69.6874	‘SiO2’
				107.6287
23	A(7)	−86.2586	CX	11.8617	108.0913	112.2249	‘SiO2’
			502.2967
24	INF	−160.0000	216.3994	REFL
	DECENTER(3)
25	INF	145.0000	C-2	REFL
26	634.1614	CX	−481.4042	CX	60.0000	311.6549	311.6673	‘SiO2’
					214.8823
27	−253.8821	CC	−610.0222	CX	25.0000	225.1467	229.7226	‘SiO2’
			153.1720
	DECENTER(4)
28	INF	−200.0000	C-3	REFL
29	823.1657 CC	353.5057	216.5542	REFL
30	103.1957	CX	77.5662	CC	25.0000	27.3671	31.8654	‘SiO2’
					145.7979
31	−1301.3477	CC	−176.7716	CX	40.0000	115.2141	127.1097	‘SiO2’
					0.1000
32	226.1976	CX	−533.9956	CX	35.0000	131.6026	129.7346	‘SiO2’
					0.1000
33	96.8063	CX	80.2315	CC	8.0304	122.5221	114.9970	‘SiO2’
	IMAGE DISTANCE =	100.0031
IMAGE	INF		108.1987
APERTURE DATA
		DIAMETER	DECENTER
APERTURE	SHAPE	X	Y	X	Y	ROTATION
C-1	RECTANGLE	52.482	20.000	0.000	25.000	0.0
C-2	RECTANGLE	329.531	50.000	0.000	−120.000	0.0
C-3	RECTANGLE	259.931	50.000	0.000	−80.000	0.0
aspheric constants
$\begin{array}{cc}Z=\frac{\left(\mathrm{CURV}\right)Y^2}{1+{\left(1-\left(1+K\right){\left(\mathrm{CURV}\right)}^2Y^2\right)}^{1/2}}& +\left(A\right)Y^4+\left(B\right)Y^6+\left(C\right)Y^8+\left(D\right)Y^{10}+\left(E\right)Y^{12}+\left(F\right)Y^{14}+\left(G\right)Y^{16}+\left(H\right)Y^{18}+\left(J\right)Y^{20}\end{array}$
		K	A	B	C	D
ASPHERIC	CURV	E	F	G	H	J
A(1)	0.851039E−02	0.00000000	−1.01624E−06	6.08007E−10	−5.62736E−13	1.14084E−15
		−2.32923E−18	2.08999E−21	0.00000E+00	0.00000E+00	0.00000E+00
A(2)	−0.618726E−02	0.00000000	1.39355E−07	1.13165E−11	7.81414E−16	5.66581E−19
		0.00000E+00	0.00000E+00	0.00000E+00	0.00000E+00	0.00000E+00
A(3)	0.518760E−02	0.00000000	−8.99477E−08	−2.67713E−12	−8.56400E−16	7.98734E−20
		0.00000E+00	0.00000E+00	0.00000E+00	0.00000E+00	0.00000E+00
A(4)	0.01015569	0.00000000	−1.65154E−06	−2.76782E−10	1.94297E−13	−5.45936E−17
		8.17140E−21	−4.67186E−25	0.00000E+00	0.00000E+00	0.00000E+00
A(5)	0.01015569	0.00000000	−1.65154E−06	−2.76782E−10	1.94297E−13	−5.45936E−17
		8.17140E−21	−4.67186E−25	0.00000E+00	0.00000E+00	0.00000E+00
A(6)	0.518760E−02	0.00000000	−8.99477E−08	−2.67713E−12	−8.56400E−16	7.98734E−20
		0.00000E+00	0.00000E+00	0.00000E+00	0.00000E+00	0.00000E+00
A(7)	−0.960266E−02	0.00000000	2.22077E−08	1.44665E−12	1.43851E−16	1.09803E−20
		0.00000E+00	0.00000E+00	0.00000E+00	0.00000E+00	0.00000E+00
SPECIAL SURFACES (SPS types)
QCN SURFACES
x = (Y/NRADIUS)**2
$\begin{array}{cc}Z=\frac{\left(\mathrm{CURV}\right)Y^2}{1+{\left(1-\left(1+K\right){\left(\mathrm{CURV}\right)}^2Y^2\right)}^{1/2}}& +x^2*\left(\left(\mathrm{QC}4\right)Q_0^{\mathrm{con}}\left(x\right)+\left(\mathrm{QC}6\right)Q_1^{\mathrm{con}}\left(x\right)+\dots +\left(\mathrm{QC}30\right)Q_{13}^{\mathrm{con}}\left(x\right)\right)\end{array}$
		NRADIUS (C2)
		QC10 (C7)	K (C1)	QC4 (C4)	QC6 (C5)	QC8 (C6)
		QC20 (C12)	QC12 (C8)	QC14 (C9)	QC16 (C10)	QC18 (C11)
ASPHERIC	CURV	QC30 (C17)	QC22 (C13)	QC24 (C14)	QC26 (C15)	QC28 (C16)
S(1)	−0.193296E−01	0.241104E+02	0.000000E+00	0.102350E+01	−0.110831E+00	−0.153148E−01
		0.409086E−02	−0.809714E−03	0.125654E−03	−0.792809E−04	0.106091E−04
		−0.131607E−04	−0.914150E−06	−0.301755E−05	−0.558949E−06	−0.106807E−05
		−0.437373E−06
S(2)	−0.549169E−02	0.410514E+02	0.000000E+00	0.647857E+00	−0.579468E−01	−0.149522E+00
		−0.563430E−01	−0.119113E−01	−0.815318E−02	−0.237721E−02	−0.153527E−02
		−0.416675E−03	−0.202108E−03	−0.522481E−04	−0.187957E−04	−0.238197E−06
		0.192168E−06
S(3)	−0.611446E−02	0.480523E+02	0.000000E+00	0.212139E−01	−0.640452E+00	0.290637E+00
		0.884384E−01	0.160688E−01	−0.316193E−02	−0.469821E−02	−0.111522E−02
		0.393635E−03	0.615198E−03	0.360576E−03	0.142886E−03	0.388167E−04
		0.577816E−05
S(4)	−0.379826E−02	0.559469E+02	0.000000E+00	−0.123020E+01	−0.577347E−01	0.143110E+00
		0.581555E−01	0.175100E−01	0.874534E−02	0.409713E−02	0.198654E−02
		0.915187E−03	0.409889E−03	0.169900E−03	0.634141E−04	0.198459E−04
		0.406977E−05
S(5)	−0.546127E−02	0.430941E+02	0.000000E+00	−0.234582E+01	−0.409559E−01	0.130732E−02
		0.358234E−02	0.144329E−02	0.459955E−03	0.919185E−04	−0.551606E−05
		−0.193417E−04	−0.133179E−04	−0.696762E−05	−0.262871E−05	−0.709265E−06
		0.335430E−07
DECENTERING CONSTANTS
DECENTER	X	Y	Z	ALPHA	BETA	GAMMA
D(1)	0.0000	0.0000	0.0000	45.0000	0.0000	0.0000 (BEND)
D(2)	0.0000	0.0000	0.0000	45.0000	0.0000	0.0000 (RETU)
D(3)	0.0000	0.0000	0.0000	−45.0000	0.0000	0.0000 (BEND)
D(4)	0.0000	0.0000	0.0000	−45.0000	0.0000	0.0000 (BEND)

TABLE 2B
Monochromatic and Polychromatic Wavefront Aberrations and Corresponding Strehl Ratios of the Overall
Embodiment 200 of FIG. 2A.
	BEST INDIVIDUAL FOCUS	BEST COMPOSITE FOCUS
			SHIFT	FOCUS	RMS		SHIFT	FOCUS	RMS
FIELD	FRACT	DEG	(MM.)	(MM.)	(WAVES)	STREHL	(MM.)	(MM.)	(WAVES)	STREHL
Monochromatic rms wavefront aberrations and Strehl ratio - Wafer to field framing plane:
Variation in best individual focus shows the residual field curvature -
much reduced when compared with Dioptric design
WL = 193.3074 193.3069 193.3065 193.306 193.3057 193.3055 193.3046
WTW = 0 0 0 1 0 0 0
X	0.00	0.00	0.000000	0.005621	0.0627	0.856	0.000000	0.000129	0.0639	0.851
Y	1.00	0.00	0.000108				0.000092
X	0.50	0.00	0.000010	−0.006715	0.0254	0.975	0.000012	0.000129	0.0297	0.966
Y	1.00	0.00	0.000071				0.000091
X	0.70	0.00	0.000110	−0.001322	0.0548	0.888	0.000110	0.000129	0.0549	0.888
Y	1.00	0.00	−0.000075				−0.000071
X	1.00	0.00	0.000200	0.002878	0.0510	0.902	0.000199	0.000129	0.0514	0.901
Y	1.00	0.00	−0.000062				−0.000071
	COMPOSITE RMS FOR POSITION 1:	0.05156
Polychromatic rms wavefront aberrations and Strehl ratio - Wafer to field framing
plane:
Reduction in Strehl ratio between monochromatic and polychromatic cases represents the
contrast loss from chromatic aberrations over the spectral band
WL = 193.3074 193.3069 193.3065 193.306 193.3057 193.3055 193.3046
WTW = 11 29 60 100 69 17 5
X	0.00	0.00	0.000000	0.007964	0.0650	0.846	0.000000	0.002451	0.0662	0.841
Y	1.00	0.00	0.000105				0.000089
X	0.50	0.00	0.000008	−0.004436	0.0317	0.961	0.000010	0.002451	0.0352	0.952
Y	1.00	0.00	0.000068				0.000087
X	0.70	0.00	0.000107	0.000998	0.0584	0.874	0.000108	0.002451	0.0585	0.873
Y	1.00	0.00	−0.000077				−0.000073
X	1.00	0.00	0.000195	0.005229	0.0558	0.884	0.000194	0.002451	0.0562	0.883
Y	1.00	0.00	−0.000063				−0.000072
	COMPOSITE RMS FOR POSITION 1:	0.05526

TABLE 3A
Description of Optical Train of the Embodiment 300 of FIG. 3A.
ELEMENT	RADIUS OF CURVATURE		APERTURE DIAMETER
NUMBER	FRONT	BACK	THICKNESS	FRONT	BACK	GLASS
OBJECT	INF	1.0000			‘Water’
2	INF	−8.2303	CX	6.4351	6.5264	14.3201	‘SiO2’
				0.1435
3	S(1)	−18.8001	CX	6.7222	22.5825	27.5686	‘SiO2’
				0.1435
4	S(2)	−30.0784	CX	8.5273	35.6362	39.1897	‘SiO2’
				0.1435
5	S(3)	−38.4857	CX	9.4617	44.1620	46.6075	‘SiO2’
			APERTURE STOP	46.6075
			0.2869
6	166.3155	CX	S(4)	10.0143	49.0041	49.4058	‘SiO2’
				23.5239
7	173.2270	CX	−162.8488	CX	7.3700	54.0004	53.9884	‘SiO2’
					9.4810
8	−154.6474	CC	−86.1299	CX	8.2671	52.1115	52.1002	‘SiO2’
				0.2096
9	A(1)	−138.6302	CX	3.7500	51.9125	52.2633	‘SiO2’
				22.8744
10	71.0710	CX	535.1092	CC	6.8489	49.1146	48.1285	‘SiO2’
				57.9463
11	−54.3888	CC	A(2)	29.9969	22.0496	17.8257	‘SiO2’
				3.7833
12	−53.1248	CC	−32.8926	CX	8.9225	18.0343	19.6876	‘SiO2’
				11.1925
13	465.4200	CX	A(3)	7.3473	19.3068	19.1032	‘SiO2’
			42.9871
	DECENTER(1)
14	INF	−43.0547	C-1	REFL
15	−140.8055	CX	A(4)	−29.9980	26.7472	29.2969	‘SiO2’
				−34.1845
16	59.5352	CC	−59.2154	CC	−30.0000	24.5566	26.7873	‘SiO2’
				−13.0243
17	A(5)	−37.3543	CC	−2.5824	31.4897	31.9462	‘SiO2’
			−38.4141
18	73.1939 CC	38.4141	56.3111	REFL
19	−37.3543	CC	A(6)	2.5824	35.8758	35.8710	‘SiO2’
				13.0243
20	−59.2154	CC	59.5352	CC	30.0000	31.4408	30.6241	‘SiO2’
				34.1845
21	A(7)	−140.8055	CX	29.9980	40.2935	38.4955	‘SiO2’
			43.0547
	DECENTER(2)
				32.6896
			20.0054
22	A(8)	69.7865	CC	16.6301	21.7570	23.4641	‘SiO2’
				71.5676
23	A(9)	−47.3231	CX	10.8672	45.7252	51.0228	‘SiO2’
			787.7006
24	INF	−50.0000	237.4629	REFL
	DECENTER(3)
25	INF	150.0000	C-2	REFL
26	40540.8039	CX	−491.5484	CX	44.9407	289.1237	292.7506	‘SiO2’
					0.1000
27	540.7167	CX	−3584.5181	CX	35.0000	288.7494	285.5192	‘SiO2’
			557.4266
				30.9950
			0.0000
				30.9950
			448.8330
28	2630.2809	CX	−397.1567	CX	51.4661	192.3463	202.1249	‘SiO2’
					73.9364
29	168.9589	CX	−2918.7765	CX	76.1582	217.9061	200.8210	‘SiO2’
					7.8995
30	131.1316	CX	235.6712	CC	35.0000	166.8410	147.9259	‘SiO2’
					16.5743
31	−652.1637	CC	84.3649	CC	8.0304	147.2153	121.3181	‘SiO2’
	IMAGE DISTANCE =	144.6348
IMAGE	INF		118.7353
APERTURE DATA
		DIAMETER	DECENTER
APERTURE	SHAPE	X	Y	X	Y	ROTATION
C-1	RECTANGLE	19.328	8.000	0.000	9.000	0.0
C-2	RECTANGLE	367.770	50.000	0.000	−170.000	0.0
aspheric constants
$\begin{array}{cc}Z=\frac{\left(\mathrm{CURV}\right)Y^2}{1+{\left(1-\left(1+K\right){\left(\mathrm{CURV}\right)}^2Y^2\right)}^{1/2}}& +\left(A\right)Y^4+\left(B\right)Y^6+\left(C\right)Y^8+\left(D\right)Y^{10}+\left(E\right)Y^{12}+\left(F\right)Y^{14}+\left(G\right)Y^{16}+\left(H\right)Y^{18}+\left(J\right)Y^{20}\end{array}$
			A	B	C	D
ASPHERIC	CURV	E	F	G	H	J
A(1)	−0.788036E−02	0.00000000	−1.60680E−06	−5.71603E−10	−7.95421E−13	1.61828E−15
		−6.85051E−18	1.52500E−20	−2.15168E−23	1.70021E−26	−5.74938E−30
A(2)	0.03313618	0.00000000	−1.12080E−05	3.59225E−08	−8.31387E−11	−8.58999E−13
		3.01032E−15	6.97263E−18	0.00000E+00	0.00000E+00	0.00000E+00
A(3)	−0.01807134	0.00000000	2.44282E−07	−5.88773E−09	1.90874E−11	5.73753E−15
		0.00000E+00	0.00000E+00	0.00000E+00	0.00000E+00	0.00000E+00
A(4)	0.01839301	0.00000000	−2.40018E−06	1.13544E−09	−1.07358E−12	6.87182E−16
		0.00000E+00	0.00000E+00	0.00000E+00	0.00000E+00	0.00000E+00
A(5)	0.206863E−02	0.00000000	−1.78913E−05	1.98684E−09	2.29867E−11	−5.17522E−14
		5.67365E−17	−2.60781E−20	0.00000E+00	0.00000E+00	0.00000E+00
A(6)	0.206863E−02	0.00000000	−1.78913E−05	1.98684E−09	2.29867E−11	−5.17522E−14
		5.67365E−17	−2.60781E−20	0.00000E+00	0.00000E+00	0.00000E+00
A(7)	0.01839301	0.00000000	−2.40018E−06	1.13544E−09	−1.07358E−12	6.87182E−16
		0.00000E+00	0.00000E+00	0.00000E+00	0.00000E+00	0.00000E+00
A(8)	−0.02941486	0.00000000	−9.82126E−07	−6.38630E−09	2.82716E−11	−1.59921E−13
		0.00000E+00	0.00000E+00	0.00000E+00	0.00000E+00	0.00000E+00
A(9)	−0.02047184	0.00000000	7.86549E−08	1.18534E−10	−1.77852E−13	1.38406E−16
		0.00000E+00	0.00000E+00	0.00000E+00	0.00000E+00	0.00000E+00
SPECIAL SURFACES (SPS types)
QCN SURFACES
x = (Y/NRADIUS)**2
$\begin{array}{cc}Z=\frac{\left(\mathrm{CURV}\right)Y^2}{1+{\left(1-\left(1+K\right){\left(\mathrm{CURV}\right)}^2Y^2\right)}^{1/2}}& +x^2*\left(\left(\mathrm{QC}4\right)Q_0^{\mathrm{con}}\left(x\right)+\left(\mathrm{QC}6\right)Q_1^{\mathrm{con}}\left(x\right)+\dots +\left(\mathrm{QC}30\right)Q_{13}^{\mathrm{con}}\left(x\right)\right)\end{array}$
		NRADIUS (C2)
		QC10 (C7)	K (C1)	QC4 (C4)	QC6 (C5)	QC8 (C6)
ASPHERIC	CURV	QC20 (C12)	QC12 (C8)	QC14 (C9)	QC16 (C10)	QC18 (C11)
S(1)	−0.375089E−01	0.117087E+02	0.000000E+00	0.781699E+00	−0.111327E+00	−0.752173E−02
		0.189059E−02	−0.165226E−02	0.132330E−03	−0.400665E−04	−0.154608E−04
		0.381404E−05
S(2)	−0.108880E−01	0.189520E+02	0.000000E+00	0.179588E+00	−0.243968E+00	0.129881E+00
		−0.269953E−01	0.723456E−02	−0.134297E−02	0.138474E−03	−0.167556E−03
		0.920416E−05
S(3)	−0.123451E−01	0.220374E+02	0.000000E+00	0.673702E+00	0.232005E+00	−0.718514E−01
		0.108260E−01	−0.224315E−03	−0.855525E−03	0.320809E−04	0.801810E−04
		−0.195269E−04
S(4)	−0.810124E−02	0.230971E+02	0.000000E+00	0.101446E+01	0.356972E−01	−0.207860E−02
		0.217109E−02	0.423426E−03	0.307139E−04	−0.463203E−05	0.168129E−05
		−0.616318E−06
DECENTERING CONSTANTS
DECENTER	X	Y	Z	ALPHA	BETA	GAMMA
D(1)	0.0000	0.0000	0.0000	45.0000	0.0000	0.0000 (BEND)
D(2)	0.0000	0.0000	0.0000	45.0000	0.0000	0.0000 (RETU)
D(3)	0.0000	0.0000	0.0000	−45.0000	0.0000	0.0000 (BEND)

TABLE 3B
Monochromatic and Polychromatic Wavefront Aberrations and Corresponding Strehl Ratios of the
Catadioptric Projection Lens (I, II) of the Embodiment 300 of FIG. 3A.
	BEST INDIVIDUAL FOCUS	BEST COMPOSITE FOCUS
			SHIFT	FOCUS	RMS		SHIFT	FOCUS	RMS
FIELD	FRACT	DEG	(MM.)	(MM.)	(WAVES)	STREHL	(MM.)	(MM.)	(WAVES)	STREHL
Monochromatic rms wavefront aberrations and Strehl ratio - Wafer to SLM:
WL = 193.3074 193.3069 193.3065 193.306 193.3057 193.3055 193.3046 nm
WTW = 0 0 0 1 0 0 0
X	0.00	0.00	0.000000	0.039535	0.0022	1.000	0.000000	0.002739	0.0026	1.000
Y	1.00	0.00	−0.003775				0.000046
X	0.50	0.00	−0.000803	−0.021277	0.0008	1.000	−0.000004	0.002739	0.0011	1.000
Y	1.00	0.00	0.002507				0.000013
X	0.70	0.00	−0.001107	−0.021449	0.0017	1.000	0.000018	0.002739	0.0019	1.000
Y	1.00	0.00	0.002472				−0.000040
X	1.00	0.00	0.000754	0.014220	0.0011	1.000	−0.000008	0.002739	0.0011	1.000
Y	1.00	0.00	−0.001178				0.000014
	COMPOSITE RMS FOR POSITION 1:	0.00178
Polychromatic rms wavefront aberrations and Strehl ratio - Wafer to SLM:
Reduction in Strehl ratio between monochromatic and polychromatic cases represents the
contrast loss from chromatic aberrations over the spectral band
WL = 193.3074 193.3069 193.3065 193.306 193.3057 193.3055 193.3046
WTW = 11 29 60 100 69 17 5
X	0.00	0.00	0.000000	0.171069	0.0173	0.988	0.000000	0.133909	0.0173	0.988
Y	1.00	0.00	−0.003792				0.000067
X	0.50	0.00	−0.000805	0.110031	0.0172	0.988	−0.000011	0.133909	0.0172	0.988
Y	1.00	0.00	0.002513				0.000034
X	0.70	0.00	−0.001119	0.109673	0.0172	0.988	0.000009	0.133909	0.0172	0.988
Y	1.00	0.00	0.002497				−0.000020
X	1.00	0.00	0.000711	0.144938	0.0172	0.988	−0.000021	0.133909	0.0172	0.988
Y	1.00	0.00	−0.001111				0.000034
	COMPOSITE RMS FOR POSITION 1:	0.01723

TABLE 3C
Monochromatic and Polychromatic Wavefront Aberrations and Corresponding Strehl Ratios of the
Overall Embodiment 300 of FIG. 3A.
	BEST INDIVIDUAL FOCUS	BEST COMPOSITE FOCUS
			SHIFT	FOCUS	RMS		SHIFT	FOCUS	RMS
FIELD	FRACT	DEG	(MM.)	(MM.)	(WAVES)	STREHL	(MM.)	(MM.)	(WAVES)	STREHL
Monochromatic rms wavefront aberrations and Strehl ratio - Wafer to field framing
plane:
Variation in best individual focus shows the residual field curvature
WL = 193.3074 193.3069 193.3065 193.306 193.3057 193.3055 193.3046
WTW = 0 0 0 1 0 0 0
X	0.00	0.00	0.000000	0.041154	0.0228	0.980	0.000000	−0.002362	0.0236	0.978
Y	1.00	0.00	0.000279				0.000268
X	0.50	0.00	−0.000064	0.017039	0.0056	0.999	−0.000064	−0.002362	0.0062	0.998
Y	1.00	0.00	0.000207				0.000209
X	0.70	0.00	−0.000053	0.009362	0.0112	0.995	−0.000054	−0.002362	0.0113	0.995
Y	1.00	0.00	0.000121				0.000124
X	1.00	0.00	0.000235	−0.083257	0.0165	0.989	0.000230	−0.002362	0.0197	0.985
Y	1.00	0.00	−0.000371				−0.000364
	COMPOSITE RMS FOR POSITION 1:	0.01670
Polychromatic rms wavefront aberrations and Strehl ratio - Wafer to field framing
plane:
Variation in best individual focus shows the residual field curvature
Reduction in Strehl ratio between monochromatic and polychromatic cases represents the
contrast loss from chromatic aberrations over the spectral band
WL = 193.3074 193.3069 193.3065 193.306 193.3057 193.3055 193.3046
WTW = 11 29 60 100 69 17 5
X	0.00	0.00	0.000000	0.075248	0.0289	0.967	0.000000	0.032115	0.0295	0.966
Y	1.00	0.00	0.000307				0.000296
X	0.50	0.00	−0.000073	0.051169	0.0186	0.986	−0.000074	0.032115	0.0188	0.986
Y	1.00	0.00	0.000236				0.000238
X	0.70	0.00	−0.000067	0.043788	0.0212	0.982	−0.000068	0.032115	0.0212	0.982
Y	1.00	0.00	0.000151				0.000154
X	1.00	0.00	0.000213	−0.047939	0.0248	0.976	0.000208	0.032115	0.0270	0.972
Y	1.00	0.00	−0.000337				−0.000330
	COMPOSITE RMS FOR		0.02453
	POSITION 1:

TABLE 4A
Description of Optical Train of the Embodiment 400 of FIG. 4.
ELEMENT	RADIUS OF CURVATURE		APERTURE DIAMETER
NUMBER	FRONT	BACK	THICKNESS	FRONT	BACK	GLASS
OBJECT	INF	1.0000			‘Water’
2	INF	−8.2303	CX	6.4351	6.5264	14.3201	‘SiO2’
				0.1435
3	S(1)	−18.8001	CX	6.7222	22.5825	27.5686	‘SiO2’
				0.1435
4	S(2)	−30.0784	CX	8.5273	35.6362	39.1897	‘SiO2’
				0.1435
5	S(3)	−38.4857	CX	9.4617	44.1620	46.6075	‘SiO2’
			APERTURE STOP	46.6075
			0.2869
6	166.3155	CX	S(4)	10.0143	49.0041	49.4058	‘SiO2’
				23.5239
7	173.2270	CX	−162.8488	CX	7.3700	54.0004	53.9884	‘SiO2’
					9.4810
8	−154.6474	CC	−86.1299	CX	8.2671	52.1115	52.1002	‘SiO2’
				0.2096
9	A(1)	−138.6302	CX	3.7500	51.9125	52.2633	‘SiO2’
				22.8744
10	71.0710	CX	535.1092	CC	6.8489	49.1146	48.1285	‘SiO2’
				57.9463
11	−54.3888	CC	A(2)	29.9969	22.0496	17.8257	‘SiO2’
				3.7833
12	−53.1248	CC	−32.8926	CX	8.9225	18.0343	19.6876	‘SiO2’
				11.1925
13	465.4200	CX	A(3)	7.3473	19.3068	19.1032	‘SiO2’
			42.9871
	DECENTER(1)
14	INF	−43.0547	C-1	REFL
15	−140.8055	CX	A(4)	−29.9980	26.7472	29.2969	‘SiO2’
				−34.1845
16	59.5352	CC	−59.2154	CC	−30.0000	24.5566	26.7873	‘SiO2’
				−13.0243
17	A(5)	−37.3543	CC	−2.5824	31.4897	31.9462	‘SiO2’
			−38.4141
18	73.1939 CC	38.4141	56.3111	REFL
19	−37.3543	CC	A(6)	2.5824	35.8758	35.8710	‘SiO2’
				13.0243
20	−59.2154	CC	59.5352	CC	30.0000	31.4408	30.6241	‘SiO2’
				34.1845
21	A(7)	−140.8055	CX	29.9980	40.2935	38.4955	‘SiO2’
			43.0547
	DECENTER(2)
				32.6896
			20.0054
22	A(8)	69.7865	CC	16.6301	21.7570	23.4641	‘SiO2’
				71.5676
23	A(9)	−47.3231	CX	10.8672	45.7252	51.0228	‘SiO2’
			787.7006
24	INF	−50.0000	237.4629	REFL
	DECENTER(3)
25	INF	150.0000	C-2	REFL
26	1020.7892	CX	−440.5935	CX	44.9407	291.7619	292.3233	‘SiO2’
					86.9784
27	−282.8413	CC	−409.0313	CX	35.0000	267.7683	276.3214	‘SiO2’
			457.4266
	DECENTER(4)
28	INF	−100.0000	C-3	REFL
29	754.6155 CC	361.7155	218.6596	REFL
30	−813.6819	CC	98.9319	CC	19.7149	39.3317	49.4552	‘SiO2’
					3.9591
31	−981.5537	CC	−89.9106	CX	20.0000	50.0401	60.6842	‘SiO2’
					79.9587
32	−793.5946	CC	−101.2088	CX	23.0169	119.0006	121.4729	‘SiO2’
	IMAGE DISTANCE =	100.0000
IMAGE	INF		118.6588
APERTURE DATA
		DIAMETER	DECENTER
APERTURE	SHAPE	X	Y	X	Y	ROTATION
C−1	RECTANGLE	19.328	8.000	0.000	9.000	0.0
C−2	RECTANGLE	367.770	40.000	0.000	−160.000	0.0
C−3	RECTANGLE	312.758	60.000	0.000	−140.000	0.0
aspheric constants
$\begin{array}{cc}Z=\frac{\left(\mathrm{CURV}\right)Y^2}{1+{\left(1-\left(1+K\right){\left(\mathrm{CURV}\right)}^2Y^2\right)}^{1/2}}& +\left(A\right)Y^4+\left(B\right)Y^6+\left(C\right)Y^8+\left(D\right)Y^{10}+\left(E\right)Y^{12}+\left(F\right)Y^{14}+\left(G\right)Y^{16}+\left(H\right)Y^{18}+\left(J\right)Y^{20}\end{array}$
		K	A	B	C	D
ASPHERIC	CURV	E	F	G	H	J
A(1)	−0.788036E−02	0.00000000	−1.60680E−06	−5.71603E−10	−7.95421E−13	1.61828E−15
		−6.85051E−18	1.52500E−20	−2.15168E−23	1.70021E−26	−5.74938E−30
A(2)	0.03313618	0.00000000	−1.12080E−05	3.59225E−08	−8.31387E−11	−8.58999E−13
		3.01032E−15	6.97263E−18	0.00000E+00	0.00000E+00	0.00000E+00
A(3)	−0.01807134	0.00000000	2.44282E−07	−5.88773E−09	1.90874E−11	5.73753E−15
		0.00000E+00	0.00000E+00	0.00000E+00	0.00000E+00	0.00000E+00
A(4)	0.01839301	0.00000000	−2.40018E−06	1.13544E−09	−1.07358E−12	6.87182E−16
		0.00000E+00	0.00000E+00	0.00000E+00	0.00000E+00	0.00000E+00
A(5)	0.206863E−02	0.00000000	−1.78913E−05	1.98684E−09	2.29867E−11	−5.17522E−14
		5.67365E−17	−2.60781E−20	0.00000E+00	0.00000E+00	0.00000E+00
A(6)	0.206863E−02	0.00000000	−1.78913E−05	1.98684E−09	2.29867E−11	−5.17522E−14
		5.67365E−17	−2.60781E−20	0.00000E+00	0.00000E+00	0.00000E+00
A(7)	0.01839301	0.00000000	−2.40018E−06	1.13544E−09	−1.07358E−12	6.87182E−16
		0.00000E+00	0.00000E+00	0.00000E+00	0.00000E+00	0.00000E+00
A(8)	−0.02941486	0.00000000	−9.82126E−07	−6.38630E−09	2.82716E−11	−1.59921E−13
		0.00000E+00	0.00000E+00	0.00000E+00	0.00000E+00	0.00000E+00
A(9)	−0.02047184	0.00000000	7.86549E−08	1.18534E−10	−1.77852E−13	1.38406E−16
		0.00000E+00	0.00000E+00	0.00000E+00	0.00000E+00	0.00000E+00
SPECIAL SURFACES (SPS types)
QCN SURFACES
x = (Y/NRADIUS)**2
$\begin{array}{cc}Z=\frac{\left(\mathrm{CURV}\right)Y^2}{1+{\left(1-\left(1+K\right){\left(\mathrm{CURV}\right)}^2Y^2\right)}^{1/2}}& +x^2*\left(\left(\mathrm{QC}4\right)Q_0^{\mathrm{con}}\left(x\right)+\left(\mathrm{QC}6\right)Q_1^{\mathrm{con}}\left(x\right)+\dots +\left(\mathrm{QC}30\right)Q_{13}^{\mathrm{con}}\left(x\right)\right)\end{array}$
		NRADIUS (C2)
		QC10 (C7)	K (C1)	QC4 (C4)	QC6 (C5)	QC8 (C6)
ASPHERIC	CURV	QC20 (C12)	QC12 (C8)	QC14 (C9)	QC16 (C10)	QC18 (C11)
S(1)	−0.375089E−01	0.117087E+02	0.000000E+00	0.781699E+00	−0.111327E+00	−0.752173E−02
		0.189059E−02	−0.165226E−02	0.132330E−03	−0.400665E−04	−0.154608E−04
		0.381404E−05
S(2)	−0.108880E−01	0.189520E+02	0.000000E+00	0.179588E+00	−0.243968E+00	0.129881E+00
		−0.269953E−01	0.723456E−02	−0.134297E−02	0.138474E−03	−0.167556E−03
		0.920416E−05
S(3)	−0.123451E−01	0.220374E+02	0.000000E+00	0.673702E+00	0.232005E+00	−0.718514E−01
		0.108260E−01	−0.224315E−03	−0.855525E−03	0.320809E−04	0.801810E−04
		−0.195269E−04
S(4)	−0.810124E−02	0.230971E+02	0.000000E+00	0.101446E+01	0.356972E−01	−0.207860E−02
		0.217109E−02	0.423426E−03	0.307139E−04	−0.463203E−05	0.168129E−05
		−0.616318E−06
DECENTERING CONSTANTS
DECENTER	X	Y	Z	ALPHA	BETA	GAMMA
D(1)	0.0000	0.0000	0.0000	45.0000	0.0000	0.0000 (BEND)
D(2)	0.0000	0.0000	0.0000	45.0000	0.0000	0.0000 (RETU)
D(3)	0.0000	0.0000	0.0000	−45.0000	0.0000	0.0000 (BEND)
D(4)	0.0000	0.0000	0.0000	−45.0000	0.0000	0.0000 (BEND)

TABLE 4B
Monochromatic and Polychromatic Wavefront Aberrations and Corresponding Strehl Ratios of the
Overall Embodiment 400 of FIG. 4.
	BEST INDIVIDUAL FOCUS	BEST COMPOSITE FOCUS
			SHIFT	FOCUS	RMS		SHIFT	FOCUS	RMS
FIELD	FRACT	DEG	(MM.)	(MM.)	(WAVES)	STREHL	(MM.)	(MM.)	(WAVES)	STREHL
Monochromatic rms wavefront aberrations and Strehl ratio - Wafer to field framing
plane:
Variation in best individual focus shows the residual field curvature - much reduced
when compared with Dioptric design
WL = 193.3074 193.3069 193.3065 193.306 193.3057 193.3055 193.3046 nm
WTW = 0 0 0 1 0 0 0
X	0.00	0.00	0.000000	0.007905	0.0078	0.998	0.000000	−0.002581	0.0079	0.998
Y	1.00	0.00	−0.000181				−0.000182
X	0.50	0.00	0.000030	−0.006455	0.0033	1.000	0.000030	−0.002581	0.0033	1.000
Y	1.00	0.00	−0.000074				−0.000074
X	0.70	0.00	−0.000008	−0.002172	0.0061	0.999	−0.000008	−0.002581	0.0061	0.999
Y	1.00	0.00	0.000032				0.000032
X	1.00	0.00	−0.000080	−0.009028	0.0040	0.999	−0.000080	−0.002581	0.0041	0.999
Y	1.00	0.00	0.000132				0.000133
	COMPOSITE RMS FOR POSITION 1:	0.00565
Polychromatic rms wavefront aberrations and Strehl ratio - Wafer to field framing
plane:
Reduction in Strehl ratio between monochromatic and polychromatic cases represents the
contrast loss from chromatic aberrations over the spectral band
WL = 193.3074 193.3069 193.3065 193.306 193.3057 193.3055 193.3046 nm
WTW = 11 29 60 100 69 17 5
X	0.00	0.00	0.000000	0.041360	0.0188	0.986	0.000000	0.030520	0.0189	0.986
Y	1.00	0.00	−0.000182				−0.000182
X	0.50	0.00	0.000030	0.026927	0.0175	0.988	0.000030	0.030520	0.0175	0.988
Y	1.00	0.00	−0.000074				−0.000074
X	0.70	0.00	−0.000008	0.030934	0.0181	0.987	−0.000008	0.030520	0.0181	0.987
Y	1.00	0.00	0.000032				0.000032
X	1.00	0.00	−0.000081	0.023475	0.0175	0.988	−0.000081	0.030520	0.0175	0.988
Y	1.00	0.00	0.000134				0.000134
	COMPOSITE RMS FOR POSITION 1:	0.01801

In one specific implementation of the projection optical system of the invention, the catadioptric projection lens is made to include first and second portions (such as, for example, portions I and II of the embodiment 200) such that the second portion is structured as a catadioptric optical system forming, in light received from the catadioptric illumination relay lens, an intermediate optical image at a location between elements of the second portion. In such specific implementation, the first portion of the catadioptric projection lens is structured as a dioptric optical unit disposed to transfer light from the location of the intermediate image to an image plane of the projection optical system to form of the intermediate optical image at the image plan. Such specific catadioptric projection lens is configured to satisfy a condition of

$\begin{array}{cc}A<\frac{{\beta }_I}{{\beta }_T}<B,& \left(1\right)\end{array}$

where β_I denotes a magnification of the first portion of the catadioptirc projection lens, β_T denotes a magnification of the whole catadioptric projection lens, A=4, B=30. As would be appreciated by a person of skill in the art, this implementation possesses an unexpected operational advantage over a catadioptric projection lens of a related art in that it avoids a situation of

$\frac{{\beta }_I}{{\beta }_T}>30,$

when the required value of the NA of the second portion is too large for practical purposes such that correction of aberrations of the catadioptric projection lens becomes prohibitively expensive. At the same time, by keeping the ratio of

$\frac{{\beta }_I}{{\beta }_T}$

above 4, the magnification value of the first portion is keep from becoming so impractically large as to make it cost prohibitive to correct aberrations of the projection optical system. It may be preferred to set A=5 and B=25 for high optical performance of the projection optical system; and even more preferred to set B=21.

In another related specific implementation of the projection optical system of the invention, the catadioptric projection lens is structured to include first and second portions as discussed above and to satisfy a condition of

$\begin{array}{cc}C<\frac{{\beta }_{\mathrm{II}}}{{\beta }_T}<D,& \left(2\right)\end{array}$

where β_I denotes a magnification of the first portion of the catadioptric projection lens and C=6 and D=20. As would be appreciated by a person of skill in the art, this implementation possesses an unexpected operational advantage over a catadioptric projection lens of a related art in that it avoids a situation when the total length of the second portion is prohibitively large from the operational standpoint and when the magnification of the first portion is too high. (Such impractical situation corresponds to D>20 and is accompanied by aberrations of the projection optical system that are too high to correct at operationally reasonable cost.) At the same time, this specific implementation is operationally advantageous over the similar system characterized by

$C<\frac{{\beta }_{\mathrm{II}}}{{\beta }_T}$

where C<6, for which the value of NA of the second portion is so high that the resulting aberrations are impractical to correct. For high optical performance of the projection optical system of the invention, it may be preferred to set C=5; to improve the operational characteristics even further, the lower limit of condition (2) may be set to 7.7. yet in a more preferred embodiment, the upper limit D may be set to 14.

In yet another related specific implementation of the projection optical system of the invention, the catadioptric projection lens is structured to include a first and second portions as discussed above and to satisfy a condition of

|β_II|<|β_I|,  (3)

to ensure high optical performance in conjunction with the digital scanner as disclosed above.

The following Table 5 illustrates non-limiting examples pertaining to configurations of the catadioptric projection lens of the projection optical system of the invention:

	TABLE 5
	Condition	Example A	Example B	Example C	Example D
	|β1|	0.1	0.1	0.1	0.1
	|β11|	0.2	0.2	0.05	0.05
	|βT|	0.02	0.02	0.005	0.005
	|β1|/|βT|	5	5	20	20
	|β11|/|βT|	10	10	10	10

An example of forming an optical image with an embodiment of the projection optical system according to the invention is schematically illustrated by a flow-chart 1000 in FIG. 10. At step 1010, radiation that has been transmitted through a catadioptric illumination relay system structured according to an embodiment of the invention as discussed above is received with an SLM. At step 1020, radiation received by the SLM through a catadioptric projection lens of the embodiment is reflected by the SLM to form an image such that chromatic errors induced in the image are at least partially reduced. As a result of such reflection, an intermediate image of an object irradiated with the radiation can be formed within the catadioptric projection lens (for example, between the elements of such lens). The intermediate image is further re-imaged, at step 1030, through the catadioptric projection lens and fluid or liquid to form as image of the object at the image plane. Optionally, at step 1040, a beam defined by the radiation received at the SLM, is digitally scanned (for example, with a digital scanner system used in conjunction with the embodiment). The radiation at hand may have a bandwidth on the order of 1 picometer, in one implementation from about half a picometer to several picometers (for example, 5 picometers).

It is notable, that a second portion of a catadioptric projection lens of an embodiments of the invention includes the combination of the two negative lenses 16, 17 (see, for example, the portion labeled II in the embodiment of FIG. 2A or that of FIG. 4, the projection lens of which is structured in a similar fashion) and, for that reason, is configured differently from similar portion that related art has been utilizing to date. In particular, catadioptric projection lenses of the projection systems of the related art include only one, single lens in place of the combination of lenses 16, 17 used herein. Such single lens is known to some as a Schupmann lens, which conventionally, is a single negative-power meniscus lens element placed close to a concave mirror of the projection lens. According to the idea of the present invention, two such lens elements are used instead, which provides the proposed designed with more degrees of freedom for correction of aberrations, in particular spherical aberration and coma. (For proper comparison of the operation of the embodiments of FIGS. 2A, 2B and 4 with projection systems of FIGS. 1A-1C and 3A-3C that are structured conventionally, the combination of two negative-power meniscus elements in used in each of the corresponding catadioptric projection lens. See also data in the Tables.)

The embodiments discussed above may be employed with an exposure apparatus that is disclosed, for example, in U.S. Pat. No. 8,089,616, and U.S. Patent Application Publications Nos. 2013/0278912, 2013/0314683, 2013/0222781, and 2014/0320835. The disclosure of each of these patent documents is incorporated by reference herein. The discussed embodiments may be also utilized in a polarization illuminating optical system that is disclosed in, for example, U.S. Patent Application Publications Nos. 2013/0146676, 2014/0211174, and 2014/0233008. The disclosure of each of these patent documents is also incorporated by reference herein.

It is appreciated that either of the illumination optical system, or the projection optical system of the embodiments discussed above, and the exposure apparatus is produced by assembling various subsystems including the constituent elements and units recited in the appended claims so that the predetermined mechanical accuracy, the accuracy of electrical and optical performance of the resulting assembly are maintained. In order to ensure such accurate operational performance, various operational adjustments may be carried out before and/or after the assembly has been completed, including adjustments for achieving the required optical accuracy for various optical elements and systems, adjustments for achieving the required mechanical accuracy for various mechanical systems, and adjustments for achieving the required electrical accuracy for various electrical systems. The steps of assembling various subsystems into the exposure apparatus include, for example, establishing mechanical connections among the components, establishing wiring connections among the electric circuits, and establishing piping connections effectuating air pressure circuits among the various subsystems. The assembling process of the individual subsystems is performed before the assembly of various subsystems into the overall exposure apparatus. When the assembly of the exposure apparatus is completed, the overall adjustment procedure is effectuated to secure the accurate operational performance of the entire exposure apparatus. It is also appropriate for the exposure apparatus to be produced in a clean room in which, for example, the temperature and the purity of environment are managed.

Embodiments of the present invention are not limited for use with an exposure apparatus configured to produce a semiconductor device, but are also widely applicable, for example, to an exposure apparatus configured to produce a liquid crystal display device formed on a rectangular glass plate, or a display apparatus such as the plasma display, as well as an exposure apparatus configured to produce an the image-pickup device (for example, a CCD), a micromachine, a thin-film magnetic head, and a DNA chip. Embodiments of the present invention can also be employed at the exposure step to be used when the mask (such as a photomask and/or a reticle) formed with the mask-pattern is produced photolithographically.

In the embodiments described above, a used light source may be configured, in a specific case, to emit UV light at a wavelength of 193 nm and a spectral bandwidth on the order of 0.1 pm (measured as full-width-half-maximum, or FWHM, value). Generally, however, another appropriate laser light source may be employed, including, for example, an ArF excimer laser source for supplying the laser beam at 193 nm, an KrF excimer laser light for supplying the laser beam at 248 nm, an F₂ laser light source for supplying the laser beam at 157 nm, the pulsed laser light source such as the Ar₂ laser (with output wavelength of 126 nm), a Kr₂ laser (with output wavelength of 146 nm), the g-ray source (wavelength of 436 nm), an YAG laser cooperated with a light-harmonic generator, and an ultra-high pressure mercury lamp configured to generate at 365 nm. As disclosed in the U.S. Pat. No. 7,023,610, it is also appropriate to use a harmonic wave as the vacuum ultraviolet light (such harmonic wave being obtained by i) amplifying a single wavelength laser beam in the infrared or visible spectral region produced by a fiber laser or a DFB semiconductor laser with, for example, a fiber amplifier doped with erbium and/or ytterbium and ii) performing the wavelength conversion into the ultraviolet spectral region by using principles of non-linear optics, for example utilizing a nonlinear optical crystal. The disclosure of U.S. Pat. No. 7,023,610 is incorporated by reference herein.

References made throughout this specification to “one embodiment,” “an embodiment,” “a related embodiment,” or similar language mean that a particular feature, structure, or characteristic described in connection with the referred to “embodiment” is included in at least one embodiment of the present invention. Thus, appearances of these phrases and terms may, but do not necessarily, refer to the same implementation. It is to be understood that no portion of disclosure, taken on its own and in possible connection with a figure, is intended to provide a complete description of all features of the invention.

It is also to be understood that no single drawing is intended to support a complete description of all features of the invention. In other words, a given drawing is generally descriptive of only some, and generally not all, features of the invention. A given drawing and an associated portion of the disclosure containing a description referencing such drawing do not, generally, contain all elements of a particular view or all features that can be presented is this view, for purposes of simplifying the given drawing and discussion, and to direct the discussion to particular elements that are featured in this drawing. A skilled artisan will recognize that the invention may possibly be practiced without one or more of the specific features, elements, components, structures, details, or characteristics, or with the use of other methods, components, materials, and so forth. Therefore, although a particular detail of an embodiment of the invention may not be necessarily shown in each and every drawing describing such embodiment, the presence of this detail in the drawing may be implied unless the context of the description requires otherwise. In other instances, well known structures, details, materials, or operations may be not shown in a given drawing or described in detail to avoid obscuring aspects of an embodiment of the invention that are being discussed.

The invention as recited in claims appended to this disclosure is intended to be assessed in light of the disclosure as a whole, including features disclosed in prior art to which reference is made.

While the description of the invention is presented through the above examples of embodiments, those of ordinary skill in the art understand that modifications to, and variations of, the illustrated embodiments may be made without departing from the inventive concepts disclosed herein. The invention should not be viewed as being limited to the disclosed examples.

Claims

1. A projection optical system configured to form an image on an image plane, comprising: 4 <  β I   β T  < 30, wherein βI denotes a magnification of the first portion and βT denotes a magnification of the catadioptric projection lens.

a catadioptric projection lens including first and second portions in optical communication with one another;

said second portion configured as a catadioptric optical system designed to form an intermediate optical image at a location between elements of the second portion;

said first portion configured as a dioptric optical system disposed to transfer light from said location to the image plane of the projection optical system to form the image thereon,

said catadioptric projection lens configured to satisfy a condition of

2. A projection optical system according to claim 1, further comprising a catadioptric illumination relay lens and a spatial light modulator (SLM) positioned to receive light from the catadioptric illumination relay lens and reflect said light towards the catadioptric projection lens.

3. A projection optical system according to claim 1, 6 <  β II   β T  < 20, wherein βII denotes a magnification of the second portion and βT denotes a magnification of the catadioptric projection lens.

said catadioptric projection lens is configured to satisfy a condition of

4. A projection optical system according to claim 1,

wherein said catadioptric projection lens is configured to satisfy a condition of |βII|<|βI|, wherein βI denotes a magnification of the first portion and βII denotes a magnification of the second portion.

5. A projection optical system according to claim 1,

wherein said second portion configured such that said light directed through the projection optical system towards the image plane passes through a first group of lenses including a first negative lens, then through a second group of lenses, and then is reflected with a concave mirror to form a reflected beam transmitted through the second group of lenses.

6. A projection optical system according to claim 5, wherein the second group of lenses includes second and third negative lenses immediately adjacent to one another, a concave surface of the second negative lens facing away from the concave mirror, a concave surface of the third negative lens facing the concave mirror.

7. A projection optical system according to claim 6, wherein the second group of lenses further comprises a positive lens between the first group of lenses and the third negative lens.

8. A projection optical system according to claim 1, wherein the first portion comprises at least two positive lenses disposed immediately adjacent to one another such as to receive light directly from said location.

9. A projection optical system according to claim 8, wherein the first portion further comprises at least two negative lenses disposed immediately adjacent to one another between said at least two positive lenses and the image plane.

10. A projection optical system according to claim 9, wherein the first portion further comprises a light-condensing lens unit between the at least two negative lenses and the image plane.

11. A projection optical system according to claim 10, wherein every lens of the light-condensing lens-unit is a positive lens.

12. A projection optical system according to claim 1, characterized, in operation with light having a central wavelength of about 193.3 nm and a spectral bandwidth of about 1 picometer, a first Strehl ratio at the central wavelength and a second Strehl ratio across the spectral bandwidth, both the first and second Strehl ratios exceeding 0.95.

13. A projection optical system according to claim 1, configured to form the image with a reduction ratio of at least 50.

14. An exposure apparatus configured to expose a substrate to light delivered thereto through liquid from an object, said exposure apparatus comprising:

a stage configured to support of a substrate defining the image plane; and

the projection optical system according to claim 1, said projection optical system configured to form said image on the substrate with light transmitted from an object through the projection optical system and liquid below the projection optical system.

15. An exposure apparatus according to claim 14, further comprising a illumination relay lens disposed to illuminate the object with light passing therethrough.

16. An exposure apparatus according to claim 15, wherein said illumination relay lens includes a catadioptric illumination relay lens.

17. A method for manufacturing a device, the method comprising:

exposing a substrate with light delivered thereto from an object through liquid with the use of the projection optical system according to claim 1, and

developing said substrate after exposure with said light.

18. A projection optical system configured to form an image on an image plane, comprising: 6 <  β II   β T  < 20, wherein βII denotes a magnification of the second portion and βT denotes a magnification of the catadioptric projection lens.

a catadioptric projection lens including first and second portions in optical communication with one another;

said second portion configured as a catadioptric optical system including a concave mirror positioned to form an intermediate optical image at a location between elements of the second portion;

said first portion configured as a dioptric optical system disposed to transfer light from said location to an image plane of the projection optical system to form the image thereon;

said catadioptric projection lens configured to satisfy a condition of

19. A projection optical system according to claim 18, further comprising a catadioptric illumination relay lens and a spatial light modulator (SLM) positioned to receive light from the catadioptric illumination relay lens and reflect said light towards the catadioptric projection lens.

20. A projection optical system according to claim 18, wherein said catadioptric projection lens configured to satisfy a condition 4 <  β I   β T  < 30, wherein βI denotes a magnification of the first portion.

21. A projection optical system according to claim 20, wherein said catadioptric projection lens is configured to satisfy a condition of |βII|<|βI|.

22. A projection optical system according to claim 18, characterized, in operation with light having a central wavelength of about 193.3 nm and a spectral bandwidth of about 1 picometer, a first Strehl ratio at the central wavelength and a second Strehl ratio across the spectral bandwidth, both the first and second Strehl ratios exceeding 0.95.

23. A projection optical system configured to form an image on an image plane, comprising:

a catadioptric projection lens including first and second portions in optical communication with one another;

said second portion configured as a catadioptric optical system that includes first and second negative lenses and a concave mirror to form an intermediate optical image at a location between elements of the second portion;

said first portion configured as a dioptric optical system disposed to form an image of said intermediate optical image at the image plane;

wherein the first negative lens has concave and convex surfaces, said concave surface of the first negative lens facing away from the concave mirror; and

wherein a concave surface of the second negative lens is immediately adjacent to the concave mirror.

24. A projection optical system according to claim 23,

wherein said second portion is positioned such that light directed through the projection optical system towards the image plane passes through the first negative lens, then through a second negative lens, and then is reflected with a concave mirror to form a reflected beam further transmitted sequentially through the second and first negative lenses.

25. A projection optical system according to claim 23, wherein the first portion comprises at least two positive lenses disposed immediately adjacent to one another such as to receive light directly from said location.

26. A projection optical system according to claim 25, wherein the first portion further comprises at least two negative lenses disposed immediately adjacent to one another between said at least two positive lenses and the image plane.

27. A projection optical system according to claim 26, wherein the first portion further comprises a light-condensing lens unit between the at least two negative lenses and the image plane.

28. A projection optical system according to claim 27, wherein every lens of the light-condensing lens-unit is a positive lens.

29. A projection optical system according to claim 23, characterized, in operation with light having a central wavelength of about 193.3 nm and a spectral bandwidth of about 1 picometer, a first Strehl ratio at the central wavelength and a second Strehl ratio across the spectral bandwidth, both the first and second Strehl ratios exceeding 0.95.

30. A projection optical system according to claim 23, configured to form the image with a reduction ratio of at least 50.